The role of the $\omega(4S)$ and $\omega(3D)$ states in mediating the $e^+e^-\to \omega\eta$ and $\omega\pi^0\pi^0$ processes
Qin-Song Zhou, Jun-Zhang Wang, and Xiang Liu

TL;DR
This paper investigates how the $ ext{ω}(4S)$ and $ ext{ω}(3D)$ states contribute to the processes $e^+e^- o ext{ωη}$ and $e^+e^- o ext{ωπ}^0 ext{π}^0$, explaining enhancement structures around 2.2 GeV observed at BESIII.
Contribution
It introduces the roles of $ ext{ω}(4S)$ and $ ext{ω}(3D)$ states in these processes, clarifying the resonance structures and differences in line shapes, supported by theoretical $ ext{ω}$ mesonic spectroscopy.
Findings
$ ext{ω}(4S)$ dominates $e^+e^- o ext{ωη}$ process.
Both $ ext{ω}(4S)$ and $ ext{ω}(3D)$ contribute similarly in $e^+e^- o ext{ωπ}^0 ext{π}^0$.
The study offers a solution to the resonance parameter discrepancy around 2.2 GeV.
Abstract
The and processes are ideal platforms to search for higher states. Focusing on the observations of two enhancement structures around 2.2 GeV existing in and at BESIII, we analyze how the and states play the role in the and processes. The present study is supported by theoretical mesonic spectroscopy. For reproducing the data of the cross sections of and , the intermediate and should be introduced, which indicates that the enhancement structures around 2.2 GeV existing in and contain the and signals. Nonetheless, in the process , the…
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Taxonomy
TopicsStochastic processes and financial applications · Quantum chaos and dynamical systems · advanced mathematical theories
